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Construction of blowup solutions for Liouville systems

Zetao Cheng, Haoyu Li, Lei Zhang

TL;DR

This work establishes the existence of multi-bubble blowup solutions for a general Liouville system on a flat torus with nonnegative, invertible, symmetric interaction matrix $A$. It develops a refined Lyapunov–Schmidt reduction combined with Fourier analysis to convert the infinite-dimensional PDE problem into a finite-dimensional problem governing bubble locations and scales, under minimal structural assumptions. The analysis yields sharp blowup profiles, detailed interaction terms, and a robust invertibility framework for the linearized operator, enabling the construction of $N$-bubble configurations in full generality. The results generalize prior one- and few-bubble constructions to arbitrary component counts, providing a systematic method to realize bubbling phenomena in Liouville systems with rich coupling behavior and geometric-analytic significance.

Abstract

We study the following Liouville system defined on a flat torus \begin{equation} \left\{ \begin{array}{lr} -Δu_i=\sum_{j=1}^n a_{ij}ρ_j\Big(\frac{h_j e^{u_j}}{\int_Ωh_j e^{u_j}}-1\Big),\nonumber \\ u_j\in H_{per}^1(Ω)\mbox{ for }i\in I=\{1,\cdots,n\}\nonumber, \end{array} \right. \end{equation} where $h_j\in C^3(Ω)$, $h_j>0$, $ρ_j>0$ and $u=(u_1,..,u_n)$ is doubly periodic on $\partialΩ$. The matrix $A=(a_{ij})_{n\times n}$ satisfies certain properties. One central problem about Liouville systems is whether multi-bubble solutions do exist. In this work we present a comprehensive construction of multi-bubble solutions in the most general setting.

Construction of blowup solutions for Liouville systems

TL;DR

This work establishes the existence of multi-bubble blowup solutions for a general Liouville system on a flat torus with nonnegative, invertible, symmetric interaction matrix . It develops a refined Lyapunov–Schmidt reduction combined with Fourier analysis to convert the infinite-dimensional PDE problem into a finite-dimensional problem governing bubble locations and scales, under minimal structural assumptions. The analysis yields sharp blowup profiles, detailed interaction terms, and a robust invertibility framework for the linearized operator, enabling the construction of -bubble configurations in full generality. The results generalize prior one- and few-bubble constructions to arbitrary component counts, providing a systematic method to realize bubbling phenomena in Liouville systems with rich coupling behavior and geometric-analytic significance.

Abstract

We study the following Liouville system defined on a flat torus \begin{equation} \left\{ \begin{array}{lr} -Δu_i=\sum_{j=1}^n a_{ij}ρ_j\Big(\frac{h_j e^{u_j}}{\int_Ωh_j e^{u_j}}-1\Big),\nonumber \\ u_j\in H_{per}^1(Ω)\mbox{ for }i\in I=\{1,\cdots,n\}\nonumber, \end{array} \right. \end{equation} where , , and is doubly periodic on . The matrix satisfies certain properties. One central problem about Liouville systems is whether multi-bubble solutions do exist. In this work we present a comprehensive construction of multi-bubble solutions in the most general setting.

Paper Structure

This paper contains 21 sections, 20 theorems, 415 equations, 1 figure.

Key Result

Theorem 1.1

Suppose that ($\mathcal{H}_1$) and $(A_{1})$ holds and either of the following holds Then, there exist $\rho_{\varepsilon}:=(\rho_{1,\varepsilon},\cdots,\rho_{n,\varepsilon})$ and a family of solutions $\{u_{\varepsilon}:=(u_{1,\varepsilon},\cdots,u_{n,\varepsilon})\}_\varepsilon$ to Problem (e:001) corresponding to $\rho_{\epsilon}$ such that $\rho_{i,\varepsilon}\to\rho_i^*$ ($i=1 as $\varepsil

Figures (1)

  • Figure 1: Example of profile of blowup solutions

Theorems & Definitions (36)

  • Definition 1.1
  • Theorem 1.1
  • Remark 1.2
  • Remark 1.3
  • Remark 1.4
  • Remark 1.5
  • Remark 1.6
  • Theorem 2.1
  • Corollary 2.2
  • Remark 2.3
  • ...and 26 more